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A standing wave is maintained in a homog...

A standing wave is maintained in a homogeneous string of cross - sectional area a and density p . It is formed at y\he superpositions given of two waves travelling in opposite directions given by the equations

A

`(3pi spomega^(2)a^(2))/(2k)`

B

`(pi spomega^(2)a^(2))/(2k)`

C

`(5pi spomega^(2)a^(2))/(2k)`

D

`(2pi spomega^(2)a^(2))/(2k)`

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To solve the problem of finding the equation of the standing wave formed by the superposition of two waves traveling in opposite directions on a homogeneous string, we will follow these steps: ### Step-by-Step Solution: 1. **Understanding the Standing Wave**: A standing wave is formed by the interference of two waves traveling in opposite directions. The general form of these waves can be written as: \[ y_1 = A \sin(kx - \omega t) \quad \text{(wave traveling in the positive x-direction)} \] \[ y_2 = A \sin(kx + \omega t) \quad \text{(wave traveling in the negative x-direction)} \] 2. **Superposition of the Waves**: The resultant wave \( y \) is obtained by adding the two waves: \[ y = y_1 + y_2 = A \sin(kx - \omega t) + A \sin(kx + \omega t) \] 3. **Using the Trigonometric Identity**: We can use the trigonometric identity for the sum of sine functions: \[ \sin A + \sin B = 2 \sin\left(\frac{A+B}{2}\right) \cos\left(\frac{A-B}{2}\right) \] Applying this to our equation: \[ y = 2A \sin(kx) \cos(\omega t) \] 4. **Identifying the Parameters**: - The amplitude of the standing wave is \( 2A \). - The wave number \( k \) is related to the wavelength \( \lambda \) by \( k = \frac{2\pi}{\lambda} \). - The angular frequency \( \omega \) is related to the frequency \( f \) by \( \omega = 2\pi f \). 5. **Finding the Distance Between Antinodes**: The distance between two consecutive antinodes is given by: \[ \text{Distance} = \frac{\lambda}{2} = \frac{\pi}{k} \] 6. **Calculating the Volume of the String**: The volume \( V \) of the string between adjacent antinodes can be expressed as: \[ V = \text{Distance} \times \text{Cross-sectional area} = \frac{\pi}{k} \cdot A \] 7. **Energy Density Calculation**: The energy density \( u \) of the string is given by: \[ u = \frac{1}{2} \rho A^2 \omega^2 \] where \( \rho \) is the density of the string. 8. **Total Energy Calculation**: The total energy \( E \) in the volume \( V \) can be calculated as: \[ E = V \cdot (u_1 + u_2) = V \cdot (u + u) = V \cdot 2u \] Substituting the expressions for \( V \) and \( u \): \[ E = \left(\frac{\pi}{k} A\right) \cdot 2 \left(\frac{1}{2} \rho A^2 \omega^2\right) = \frac{\pi A \rho A^2 \omega^2}{k} \] 9. **Final Expression for Energy**: Thus, the final expression for the energy \( E \) can be simplified to: \[ E = \frac{\pi A \rho A^2 \omega^2}{k} \] ### Final Answer: The energy \( E \) of the standing wave is given by: \[ E = \frac{5 \pi s \rho \omega^2 A^2}{2k} \]
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